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First Assessment Report - IPCC

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248 Dctec tion of the Gieenhouse Effec t in the Ohsei \ations 8<br />

current scientific focus in the detection issue is thereloic on<br />

multivariate or fingerprint analyses The fingerprint method<br />

is essentially a form of model validation, wheie the<br />

perturbation experiment that is being used to test the<br />

models is the currently uncontrolled emission of<br />

greenhouse gases into the atmosphere The method is<br />

discussed further in Section 8 3 <strong>First</strong>, however, we<br />

consider some of the more general issues of a detection<br />

strategy<br />

8.2 Detection Strategies<br />

8.2.1 Choosing Detection Variables<br />

There are many possible climate elements or sets of<br />

elements that we could study to try to detect an enhanced<br />

greenhouse effect In choosing the ones to study, the<br />

following issues must be considered<br />

the strength of the predicted signal and the ease with<br />

which it may be distinguished from the noise,<br />

uncertainties in both the predicted signal and the noise,<br />

and<br />

the availability and quality of suitable observed data<br />

8 2 11 Signal to noise tatios<br />

The signal-to-noise ratio provides a convenient criterion for<br />

ranking different possible detection variables The stronger<br />

the predicted signal relative to the noise, the better the<br />

variable will be for detection purposes, all other things<br />

being equal For multivariate signals, those for which the<br />

pattern of natural variability is distinctly different from the<br />

pattern of the predicted signal will automatically have a<br />

high signal-to noise ratio<br />

Signal to-noise ratios have been calculated tor a number<br />

of individual climate elements from the results of lxCCb<br />

and 2xCC>2 equilibrium experiments using atmospheric<br />

GCMs coupled to mixed-layei oceans (Bainett and<br />

Schlesinger 1987, Santer et al , 1990 Schlesinger ct al<br />

1990) The highest values were obtained lor free<br />

troposphere temperatures, near-surface tempeiatures<br />

(including sea-surface temperatures), and lower to middle<br />

troposphenc water vapour content (especially in tropical<br />

regions) Lowest values were iound for mean sea level<br />

pressure and precipitation While these results may be<br />

model dependent, they do provide a useful preliminary<br />

indicator of the relative values of different elements in the<br />

detection context<br />

Variables with distinctly difleient signal and noise<br />

patterns may be difficult to find (Bamett and Schlesinger,<br />

1987) There are reasons to expect parallels between the<br />

signal and the low-frequency noise patterns at least at the<br />

zonal and seasonal levels, simply because such char<br />

actenstics anse through feedback mechanisms that are<br />

common to both greenhouse forcing and natural variability<br />

82 I 2 Signal umeitauities<br />

Clearly a vanable toi which the signal is highly uncertain<br />

cannot be a good candidate as a detection variable<br />

Predicted signals depend on the models used to produce<br />

them Model-to-model differences (Section 5) point<br />

strongly to laige signal uncertainties Some insights into<br />

these uncertainties may also be gained from studies ol<br />

model results in attempting to simulate the present-day<br />

climate (see Section 4) A poor representation of the<br />

present climate would indicate greater uncertainty in the<br />

predicted signal (e g , Mitchell et al , 1987) Such<br />

uncertainties tend to be largest at the regional scale because<br />

the processes that act on these scales are not accurately<br />

represented or paiametenzed in the models Even if a<br />

particular model is able to simulate the present-day climate<br />

well, it will still be difficult to estimate how well it can<br />

define an enhanced greenhouse signal Nevertheless,<br />

validations of simulations ol the present global climate<br />

should form at least one of the bases for the selection of<br />

detection variables<br />

A source of unccitainty hcie is the difference between<br />

the results of equilibrium and transient experiments (see<br />

Section 6) Studies using coupled ocean-atmosphere GCMs<br />

and time-varying CO2 loicing have shown reduced<br />

warming in the aieas of deep water formation (1 e , the<br />

North Atlantic basin and around Antarctica) compared with<br />

equilibrium results (Bryan ct al , 1988, Washington and<br />

Mcehl, 1989, Stouffer et al , 1989) These experiments<br />

suggest that the regional patterns of temperature change<br />

may be more complex than those predicted by equilibrium<br />

simulations The results of equilibrium experiments must<br />

therefore be considered as only a guide to possible signal<br />

structuie<br />

The most reliable signals aie likely to be those related to<br />

the largest spatial scales Small-scale details may be<br />

eliminated by spatial averaging, or, more generally by<br />

using filters that pass only the larger scale (low wave<br />

number) components (Note that some relatively smallscale<br />

features may be appropriate for detection purposes, if<br />

model confidence is high ) An additional benefit of spatial<br />

averaging or filtenng is that it results in data compression<br />

(1 e , reducing the dimensionality of the detection variable),<br />

which facilitates statistical testing Data compression may<br />

also be achieved by using linear combinations of variables<br />

(e g , Bell, 1982, 1986, Kaioly, 1987, 1989)<br />

8 2 13 Noise unteitamties<br />

Since the expected man-made climatic changes occur on<br />

decadal and longer time-scales, it is largely the lowfrequency<br />

characteristics of natural variability that are<br />

important in defining the noise Estimating the magnitude<br />

of low frequency variability presents a major problem<br />

because of the shoitness and incompleteness of most

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